Note: Descriptions are shown in the official language in which they were submitted.
I~J~ 586 L-46a
ILINE EQUALIZER WITH DIFFER~NTIALLY CONTROLLED COMPLEMENTARY
2 ¦CONSTANT RESISTANCE NETWORKS
BACKGROUND OF INVENTION
41This invention relates to variable line equalizers and line
~¦ build-out networks tLBO s) for subscriber carrier transmission systems and
6 ¦ more particularly to such circuitry employing a pair of complementary
7 ¦ constant-resistance networks (CRN'5) that are terminated by differentially
81 controlled variable resistors.
9¦ The transmission of voice signals over subseriber car~ie~ circuits
lO¦ requires ~hat the ~ransmission characteristic of a channel, including the
11¦ communication m~dium ~hich may be a twisted-pair telephone cable, be
l2¦ sufficiently uniform that there is a minimum distortion oE information
13¦ being transmitted. It i5 well known, however, that the attenuation
141 characteristics of a telephone cabl~ change with signal frequency and the
lS¦ length of a line. It is necessary therefore to employ equalizers and/or
r 16¦ line build-out natworks to equalize the channel by introducing ertain
~ 17¦ amounts o~ a~tenuation in selected portions o~ the signal frequency spectrum
1~¦ to comyensate for the nonuniform attenuation introduced by the cable pair.
Stated differently, the attenuation characteristic of the equalizer mus~
~;20¦ be complementary ~o that of the unequalized channel so that the sum of
decibel measures of these attenuations is approximately constan~ with
22 ~requency, i.e., so tha~ the resultant at~enuation characteristic in the
2~ channel is flat. Al~hough this means that the resultant signal level is
4 reduced, this loss in signal c~n be compensated for in an ~mpliEier.
Various ~ypes o equalizers and line build-out networks have
;26 been employed or accomplishing this function. Bode-type equalizers are
27 thr~e-por~ networks which are often omployed in these applications. They
28 are described i.n patent 2,096,027 by H. W. Bode, filed January 30, 1936
29 and issued October 19J 1937, and the article, "Variable Equalizers" by
31
32 _ ~ _
;` ;
l ~ ~ 4 5 8 6 L-468
¦ H. W. Bode, pp. 229 - 244, The Bell System Technical Journal, vol. 17~
2 ¦ no. 2, April 1938. Although such equalizers often employ only passive
3 ¦ elements and a single resistor as a variable impedance element, active
Bode-type equalizers are also available as are such networks employing the
5 ¦ combination of a constant resistance network (CRN) and a variable resistor
61 as the variable impedance element. CRN's are also employed as variable
7 ¦ equaliz~rs. Such netwcrks are generally described in the Bode patsnt
8 1 2,096,027 and in th~ articles, "Disto~tion Correction in Electrical
¦ Circuits with Constant Resistance Recurrent Networks" and "Theory and
¦ Desic~n o Uniform and Composite Electric Wave Filters", both by Otto J.
ll ¦ Zobel, The Bell System Technical Journal, pp. 438 - 534, vol. 7, no. 3,
12 ¦ July 1928 and pp. 1 - 46, vol. 2, no. 1, January 1923, respectively. A
13¦ CRN is essantially a two-port network which is comprised of resistors
14 ¦ and one or more pa;rs of inverse networks of cons~ant impedance product.
151 In a CRN having one port te~minated by a resistance Ro which is equal to
18¦ this product, the image impedance across the other port is also equal to
17¦ Ro and is constant over a frequency band where the terminating resistance
18¦ remains constant and equal to Ro. In a CRN of appropriate d sign, lts
l9¦ attenuation characteristic is complementary to that o a cable pair or
201 other typ~ of transmission m~m when the former is terminated by a
21¦ resistance o~her than Ro that is related to the line length. It i~ known
22 that the variable terminating resistance of the CRN may be produced by
23 an elec~ronically con~rolled alement such as a thermistor. Such networks
24 provide a limited range of equalizc~tion. A dlfferent type of equalizer
is described in ~he U.S. patent 3,806,839 by Takuya Iwakami, filed
26 December 12, 1972 ~nd issued Aprll 23, 1974.
27
Z8
29
;30
31 3 _
32
.'
',''',
~:'',, ~ ':;;: .'
.. : .... ~. .... .
~LC16~5~36 L-468
1 ¦ S~MMARY OF INV~NTION
2 ¦ An object of this invention is the provision of an improved
31 variable equalizer circuit embodying constan~ resistance networks.
4 ¦ In accordance with this invention, an adjustable equalizer
51 comprises a circuit arrangement including first and second complementary
6 ¦ constan~ resistance ne~works in the forward gain and feedback loops,
7 ¦ respecti~ely, of an active element. The networks are te~minated by
l a~sociated variable resistance elements which are diferen~ially controlled
9 ¦ by signals that are a unction e~ the length o~ a transmission medium.
10 ¦ The impedance characteristics of the networks are additive in ~his
111 arrangement in a manner such ~hat the net gain of the active element
~21 is the inverse o~ the attenuation characteris-eic of the transmission medium,
-` 13 ¦ and the overall loss characteristic is constant.
~ ~1
15l BRIEF DESCRIPTION OF DRAWINGS
I ~
16¦ This invention will be more ~ully understood ~rom the following
17¦ detailed description of preferred embodiments thereof incorporated in a
18¦ slngle-sideband resonant-transfer subscriber carrier multiplex telephone
19¦ system wherein:
20¦ FIG. 1 is a schema~ic block and circ~it representation of
21¦ subscriber ~erminal aquipment 12 in a subscriber carrier system and
Z2 embodying this invention;
23 PIG. 2 is curYes illustrating tha attenuation characteristics
24 o a cablc pair ~ransmission line;
~IG, 3 is curvcs that are normalixed with respect to Ro and
26 which illustra~e the operation of circuitry embodying ~his invention.
27 FIG. 4 is a schematic circuit repres~ntation of a constant
28 resistance netwark 60,
Z9 FIG. S is a schematic and block diagram af the line build-out
network 40 and variable termination circuit 55 in FIG. l;
31
~2 _ ~ _
.,~ ,.,
. . - . . ~ . ......... .
: . . , .. i ; ~. . .
. - ~ " : . ~ .. . .
10~4586 L-458
1 ~ FIG. 6 is curves illustra~ing the resistanee ch~racteristics of
2 thermis~ors;
31 FIG. 7 is a de~ailed circuit diagram of one forln of the constant
4 ¦ resistance networks 71 and 72 in FIG. 5; and
5 ¦ FIG. 8 is a schematic circuit diagram of an alternate embodiment
G¦ of this invention.
7 l
8 ¦ DESCRIPTION OF PREFERRED EMBODLM~NTS
I ~
g ¦ A single-sideband1 resonant-transfer subscriber carrier multipl~x
10 ¦ system embodying this invention is describe~ in the publications,
11 ¦ "A 48-Channel Subscriber Multiplex System Using Resonant Transfer Modulation"
12 I by Lawrence E. Getgen, and "Lin0 Equipment fcr a Subscriber Multiplex
l~ ¦ Using Resonant Transfer Modulation" by Neale A. Zellmer, Conference Record
14 ¦ of the Internat;onal Conference o~ Communications ~ICC 1975), June 16-18,
151 1975 in San Francisco, Calif. J pp. 8-10 ~o 8-14 and 8-15 to 8-19, respectively.
:~ .
The subscriber terminal line equipment 12 in FIG. l for such a system is
a ¦ connected through a cabl~ pair 11, for example, to central ofice equipment
(not shown). The attenuation characteristic for line 11, when subscriber
201 termlnal 12 is located at hal~-span spacing, is represented by curve 14
21¦ in ~IG. 2. The curves 15 and 16 represant this loss charact~ris~ic when
22 the terminal 12 is spac~d at 10s5 than and greater than half-span,
23 respectively.
24 In the central office equipment of this system, low-frequency
~roup signals are generated and are transla~ed ~o high-frequency group
26 signals which are combined with a 160 kHz pilot signal. The transmission
2q ~level of this`pilot signal i5 controlled ln the central ofice so that
2~ ;it can be used to synchronize and regulate circuitry in the subscriber
29 terminal. Th~ combined high group and pilot signals are preemphasized
with hal~-sp~n slope in the central ofice prior to transmission on
31 ~
3~ ~ 5 _
~.''
~ 4 5~36 L-468
1 1 line ll ~o the equipment 12 in a subscriber terminal. This pree~phasis
2 ¦ makes it easier to later exploit the positive and negative slope control
31 of the input impedance of const~nt resistance networks ;n a variable
4 I equalizer embodying this invention~ as is described more fully hereinafter.
The su~scriber terminal 12 generally comprises a transmit sec~ion
61 21, receive sectien 22, and co~non channel signaling equipment which is
71 conventional and not shown here. In the transmit ssction 21, signals
81 from a subscriber channel and a 72-kHz pilot si~nal oscillato~ 25 are
gl combinad in a summing network 26 to produce a low-group signal on line 27.
10¦ The transmission level o~ this signal is adjusted by correla~ive control
Ill and preemphasized in a line build-out network 28, ampli~ied by circuit 31,
12¦ shaped by the 72-kHz lowpass filter 32, and transmitted on the cable
13¦ pair ll to the central office equipment. The 72-kHz pilo~ signal is
¦ extracted from ~his low-group signal in the central office and used ~o
15¦ regulate the receive levsl.
16¦ Signaling information and high-group signals on cable pair 11 are
17 collpled through hybrid 34 and are separated by the 4~k~1z lowpass ilter 35
18 ~and the -kHz highpass filter 36 and passed ther~by to associated circuitry.
19 The low-group signal from filter 32 in the ~ransmit section 21 is passed
20 ~y the highpass fil~er 36 to line 11, of course, bu~ is blockecl from ~he
21 signaling equipmant and recelve channel 22 by associat~d filters 35 and 38.
22 Finally, the high-group signal from line ll i5 also blocked from the transmit
23 section 21 by the lowpass ilter 32 and is passed to the receive section
24 22 ~y the 92-kHz high-pass ilter 38 on the input thereo.
The recelve section 22 comprises the series co~nbination of the
26 high-pass filter 38, line build-out network 40, bridging ampli~ier and phase
2~ splittsr 42~ balanc~d modula~or 46, power ampliier 49, and a channel
28 splitter network SO, or equallzing and ~e~ultiplexing r~ceived signals.
29 The receive section 22 also includes a feedbaclc network 52, which is
3~
31
32 - 6 -
.~:
',':
' ~ . ' ' ' ' ,, . ' ' '
~ lOii~5i3ti L-4~8
1 ¦ responsive .o a portion o the equalized signal on line 43 for producing
2 ¦ a 160-kHz pilot signal control voltage on line 53 and a DC error voltage
i 3 ¦ on lines 54. This error voltage on ~he lines 54 adjusts the values of
4 ¦ impedances in circuits 55 and 29 whic~ / terminations for associated
; 5 I build-out networks 40 and 28.
6 ¦ Briefly, the line build-out network 40 adjusts the level o the
.. ~ 7 ¦ high-group signal in a manner which is generally illus~rated by the curves
; 8 ¦ in FIG. 3 and described more fully heroinafter. The circuit 42 comprises
I a pair o transistor amplifiers which bridge a portion of the equalized
10 I signal on line 41 onto the output line 43 and which produces balanced
11 push-pull high-group signals on lines 44 and 45. The ~npli~ied signal
12 on line 43 is applied to a pilot pick-off amplifier 56, which includes a
13 notch filter that passes only the 160-kHz pilot signal. The amplified
14 pilot signal on line 53 is used in balanced modulator 46 to translate the
high-group signals on lines 44 and 45 back to the low-frequency group
- 16 signals which wers originally a~ailable in the central office equipment.
17 These low-group signals are amplified in circuit 49 and delivered by
1~ channel splitting ne~work S0 to associa~ed subscribeT channels. The
160-kHz signal from the pilot pick-off amplifier 56 is also rec~ified
ZO : in a linear rec~i~ier circuit representad by diode 58 and is compared
~ ~ ~ 21 with a reference voltage produced by a Zener diode S9 ~o produce the
; 22 DC error voltage signal on llnes 54, which is proportional to the langth
231 of the transmission line 11.
Z4 A constant resistance network (CRN) is basically a two-port device
having one port terminated by a variable resistor and con~rising one or
2~ more inverse impedance n~works which have iJ~ed~lces that are a function
27 of the inver~e impedances Zll and ~21 of inverse networks Zll and Z21
; Z8 which satisfy the relationship Zll ~21 ~ Ro2 for all frequencies in a
29 ~requenc~ band. A bridged T-type CRN 60 of conventional design is illustrated
30~
31~ _ 7
~ ¦ 3L~i4~3~; L-4G8
.~ I
I in schematic form in FIG. 4, corresponding la~tice-~ype CRN's also being
2 I avail~ble. The properties and desi~n of CRN's are described ln articles
31 including ~he aforementloned ones by Zobel and Bode. When one port 62 of
41 this CRN 60 is terminated in the proper load resistance R = Ro, the image
61 impedance Zi reflected across th0 network to the other port 63 is the s~ne
¦ resis~ance Ro, which is independent o ~requency across some fr~quency band,
I i.e., the impedance characteristic of the CRN 60 is flat (see curve 64 in
; 8 I FIG. 3). When the te~ninating resistance R is varied rom this value Ro,
9 ¦ the image impedance Zi vs. requency characteristic of CRN ~0 changes in a
101 prescribed and predictable manner. The curves 65 and 66 represent the
11 I input impedance of the CRN 60 as the terminating res;stanc~ decreases from
; 12¦ the value Ro ~o 0 ohms. Conversely, the curves 67 and 68 r~present the
~31 input impedance of CRN 60 as the terminating resistance is increased ~rom
1~¦ the value Ro to infinite resistance. By properly selecting values of elements
¦ making up the inverse networks Zll and Z21 and o~her elements of the CRN
161 as is known in the art, the reflected impedance Zi may be made to va~y
17¦ in a prescribed manner, which is the complemen~ of the 10%s charac~eristic
18¦ o~ a length of cable pair 11 or other type of transmission line ~curves
J 19 14 - 16 in FIG. 2). A~sociated curves 65 ~nd 67 and curves 66 and 68
illus~ra~e ~he plus and minus symmetry provided by a CRN as its termina~ing
2~ resistance is inc~eased and decreased, respectivQly, at the same rate from
22 the value Ro. It has been found that the correction provlded by a single
23 CRN is not su~icient to equaliz~ a line ll for a full span of 45 dB length.
24 In accordance with this invention, a larger ~nount of equalization
25 is obtained wi~.h ~he line build-out network tLBO) 40 and terminating circuit
26 55 in FIG. 5 ~han is available with a single CRN. As .ststed previously~
27 the sys~em employs preemphasis for half-span equaliza~ion. The LB0 40
28 here comprises a variable 8ain ~eedback stabilized amplifier 70 ~hat is
29 represented b~ the transistor Ql and a pair of constant resistance networks
32 8 -
'`'''~
,,,,
.~ , . , . : .
.. .
~ l~ti458l; L-468
1 ~CRN's~ 71 and 72 having complemen~ary impedance characteristics in the
2 forward and feedback loops, respectively, of the ~mplifier. By complementary
3 it is meant that the impedance characteristics of CRN's 71 and 72 are
4 essantially similar, although of opposite slope. An unequalized signal
51 ei on line 39 is applied to the Ql base electrode, an equalized signal eO
6~ bein~ coupled on line 41 from the Ql collector electrode. The CRN 71 has
7 an input impedance ZC looking into the one port 73 thereof, which is
connected between the Ql collector electrode and the positive supply voltage
9 ~V. The other CRN 72 has an input impedance ZE looking into the corresponding
port 75 thereof, which is connected between the Ql emit~er electrode and
11 the negativa supply voltage -V. The other ports 74 and 76 of the CRN's
~2 are terminated by elements of circuit 55.
13 The variable termination circuit 55 comprises a pair of
14 thermistors 82 and 83 in the collector circuits o associated transistors
Q2 and Q3 of a differential amplifier 80. The emitter electrodes of the
16 differen~ial amplifier 80 are driven by a cons~ant current source
17 represented by transistor Q4. The bias circuits associated with transistors
18 Ql - Q4 are omitted from FIG. 5 or simplicity of illustration. The Q2
19 base electrod~ receives the DC error voltage on line S4, which i5 produced
by recti~ication of the 160-kHz pilot signal. This error voltage is
21 proportional to the length o~ the llne 11. The Q3 base slectrode is
22 connected to ground. The collector electrodes of these transistors Q2
23 and Q3 are connected to terminals 74A and 76A of associa~ed ports of the
24 CRN's. Thus, the network~ 71 and 72 are te~ninated by the associated
thermistors 82 and 83. Since thermisto~s 82 and 83 are in the collector
Z6 circuits of transistors that are driven differentially, the collector
27 currents iC2 and ic3 in these thermistors cause ~he resistances thereof
28 to essentiaIly vary directly and inversely as the length of the line 11.
29
0 .
~ ~ ~ 32 _ 9 _
,~:
.,.
. , , ;.;: ~
I.C3t~4586 L-468
l ¦ Consider that the CRN's 71 and 72 are represented by the circuit
2 ¦ in FIG. 4 and are normalized with respect to a resistance Ro. Here,
¦ 1 2 0 ~ re Zl Zll/R0 and Z2 ~ Z2l/Ro- It can be shown in
41 this instance that the reflected impedance ZC in the collector CRN 71
51 is representable as
61 21kk ~ M
¦ ~ M~
81
where M(f~ ~ Z~Z * 2), Z = Zl ~ l/Z2~ R = kRo, and k is a variable. If
10¦ k - 1, then ZC ~ Ro/Ro ~ 1 as is expected. If tha terminating resistance
R - k'Ro for the other CRN 72, where k1 _ l/k, then it can also be shown
~21 that the reflected impedance ZE in the emitter CRN 72 ls representable as
131 ZE ~ = ZC . ~2)
1~1
16 This means that where k = 1, the networks are terminated in their
17 associated characteristic imped~nces and have input impedances represented
1~ by curve 64. ~he values of k and k' vary, of course, in order to make the
19 impedance characteristics of the two networks 71 and 72 different from the
curve 64 and the slopes thereof othqr than zero. In ~his instance, where
21 k is di~ferent rom l, the input impedances ZC and ZE of the ne~works are
22 a func~ion of frequency, i.e., they are no~ constant. The curves 66 and
23 68 illustrate t:he shape o~ the input impedance ZC ~or k < 1 and k > l,
~4 respectively. Conversely, these curves 66 and 68 illus~rate th0 shape o~
tha inpu~ imp~dance ZE or k' > l and k~ ~ 1, respectively. For
26 particular values of terminating resistances R ~ Ro such that k ~ k' ~ 1
27 and k - l/k', thcn the impedance characteristic 65, for example, o~ network
28 71 has a positiv~ slope with respect to frequency, whereas the correspondin~
29 impedance characteristic 67 of network 7~ has an equal and opposite slopa.
31
3~ - lO -
.~.
~ " ..... . .
~ 5~36 L-46d
1 1 It has been found that the impedance characteristics of the two CRN's
will be substantially complemontary, even if k' does not track l/k
3 ¦ 0xac~1y, i.e., i k' ~ l/k Eor all values ~hereof. As long as k and k'
41 move in opposite directions, the effects of CRN's 71 and 72 in LB0 40
51 are additive in some manner in the ~1 collector oircuit.
Since the feedback of amplii~r 70 is very large, t'he voltage
7 ¦ gain V.G. thereof is inversely proportional to the eedback which is
81 controlled by the impedance ZE~ i.e.g
V.G. = l/ZE. ~3)
~¦ The attenua~ion gain o the amplifier however, is directly proportional
to the impedance ZC Thus, the net voltage gain V.G.net of amplifier
12¦ 70 i5 approximately equal to the ra~io of the input impedances of networks
131 71 ~nd 72 and is reprasentable as
141 2
1~¦ V 5net = ZC/zE ~ ZC ' (4~
This means that for su~h a circuit the decibel measure of the dynamic range
17 of the LB0 40 is double that available from a single CRN. ',~here ~ - 1,
18 thPn Z~ = 1 and th~ net gain of amplifier 70 is unity. Wher~ k ~ 1, then
19 ampliier 70 effectively inverts one of the curves 65 and 67, for exsmple,
and adds them toge~her ~o produce the net gain in aquation t~). The curves
21 65 and 67, for e~ample, also generally illustrate a ne~ positive gain and
~2 net sttenuation ~or negative gain), respectively; provided by amplifier 70.
23 Since the subscribe~ terminal 1~ and LB0 40 are preemphasized
24 for half-span spacin~, only '~ half-span compensation is required for
full-span eq~allzation. It is then possible ~o loca~e a subscribsr
26 terminal at a spacing o ~ half-span from the hal-span location and still
2~ obtain the desir~d equalization. With two CRN's in the LB0 40 here, each
28 of the CRN's 71 and 72 need only provide ' quarter-span compensation.
2g Noting the plus/minus symmetry of the impedance charactsris~ics o ~he
31 - 11
32
,~,
r~ j ~ , ; ' , :
~ ~S~j4 5 ~j L-468
1 ¦ CRN's, it is seen that the LBO 40 truly provides gain in both directions
2 ¦ (i.e., either gain or attenuation) as is requi-red for effecting the
3 ¦ desired au~omatic equalization in a system where a subscriber terminal 12
4 ¦ is l~cated at + half-span from the half-span location.
5 ¦ When appropriat0 values of elements of the CRN's 71 and 72 are
6 ¦ chosenJ the shapes of the impedance characteristics t~ereof will be similar
7 ¦ to that of line 11 such that the decibel measure of the net line 10s5
¦ ~including preemphasis) will be substantially the complement o~ the sum
¦ of the d~cibel measure of the impedance charac~eristic of CRN 71 and the
10 ¦ reciprocal of the impcdance characteristic of CRN 72. ~his design is
Il ¦ accomplished in practice by first measuring the loss charact0ristic of a
12 ¦ particular transmission line 11 as a ~unction o frequency. Constant
13 ¦ resistance networks are then designed having a prescribed characteristic
1~ ¦ impedance and having impedance characteristics that ~rack the line loss
15 ¦ charac~eristic or some values of terminating resistance. Finally, an
16 ¦ electrically variable resistive element, or example, having a resistance
17 ¦ which varies as a ~unction o a control signal that is proportional ~o
¦ the length o~ line 11 at some rate is selected. Such an element may,
19 ¦ for example, be one or more ~hermistors or semiconductor diodes.
ZO ¦ The description in the ~irst three of the ~our preceding paragraphs
21 ¦ was~essentially based on the assumption that ~ho CRN's 71 and 72 have
22 ¦ ~erminating resistances that vary reciprocally f.rom a value R = Ro for
23 ¦ whîch the impedance characteristic of each network is 1at, see curve 64.
24 ¦ The resistanc~s provided by thermistors9 however, vary with control
25 ¦ current in a ~anner shown ln FIGo 6. The curves 92 and 93 represent
28 ¦ the impedance characteristics of the~mistors 82 and 83, respectively, in
27 ¦ FIG. 5. Although the resistance provided by one thermistor increases as
28 ¦ the resistance provide~ by the other decreases~ they do not necessarily
29 ¦ track ~ach other such that the rasistance o~ thermistor 82 is always equal
31 ¦ to the r~ciprocal of the resistance of thermistor 83. In arriving a~ an
~2 ~
I
j~ ~ ' I
~ L-~6
1 I.BO 40 in a practical implementation of this invention, the CRN~s 71 and
2 72 are designed to have a prescribed characteristic irnpedance that tracks
3 the loss characteristic of line ll or some terminating resistance between
4 the minimum and maximum values theraof that are obtainable from a
5 thermistor having a desired dynamic range in the order of about 23 dB.
Maximum and minimum resistances of the thermistors are selec~ed ~or a
nominal minimum current iC3(min) a~ the maximum ambient temperature to be
encountered and for a nominal maximum current iC3~max), respectively. The
9 characteristic impedances Ro o the CRN's are approximately equal to the
geometric mean between these minimum and maximum resistances of the
11 thermistors. The resistances of the two thermistors are the same values Re
lZ or~the error signal voltage e54 ~ O. Although the impedance characteristic
13 o the two CRN's will not be 1at when the ~erminating resistances are
14 the same value Re for e54 = O ~olts, they will be the same shape and have
slopes of the same sign. Thus 9 when the~e two impedance characteristics
16 are combined in amplifier 70 according to equation ~4), the net voltage-gain
1~ of the ampli~ier will be flat. As the resistances of ~he thermistors
18 v~ry rom this value R~ the impedance characteristics of the networks
l9 move in opposîte directions such that the net gain of the ampllfier still
tracks the loss characteristic of line 11 and provides the desired equalization
~1 In a line build-out network that was built and successfully
22 operated, CRN's 71 and 72 were bridged T devices o~ tha type illustra~ed
23 in PIG. 4 and shown in detail in FIG. 7. Each CRN provided corraction in
24 one direction fo:r a quarter-span spacing. Thus, two CRN's usable in both
direc~ions (both providing plus and minus galn), where there is hal-span
~6 preemphasis, provide ~or full-span e~ualiza~ion. Th0 ~wo CRN's 71 and 72
2~' in this LBO were identical. The resistors Rl and R2 were the resistors in
28 the series arm o the T-structure having values that are equal to the
29 resistance Ro. The bridg:ing network Zll comprised the parallel combination
32 - 13 -
, ~
,. ,,, ~ . .. . .
58~i ~
L-46~
1 of a capacitor Cl an~ resistor R3. ~he inYerse network ~21 in the shunt arm
2 of the T-structure comprised the resistor R4 and inductor Bl, which were
connected in s~ries. The one-por~ 62 of the network was terminated by a
4 variable resistor R5, which was a thermistor. A capacitor C2 was connected
between one side of thermis~or R5 ancl the bridging network Zll to block
6 DC current. A resistor R6 was effect:ively connecte~ in shunt ~ith
7 thermistor R5 to limi~ the maximwm attainable t~rmination resistance.
In this LB0 40, the terminals 63A of the other port 63 of networks 71 and
9 72 were connected to the Ql collector and emitter electrodes, respectively.
The other terminals 63B thereof were connected to associated supply
11 voltages. The networks 71 and 72 in this LBO~ for operating over a
12 frequency band of 92 - 160 kHz on 22-gauge twisted-pair telephons cable
1~ had the following element values:
14 Rl 909 ohms
~2 909 ohms
16 Cl 0.01 microfarads
17 R3 562 ohms
18 R4 1470 ohmc
19 Ll 8 millihenries
2~ ~ R5 Ro = 909 ohms
21 , Rmin 200 ohms
22 ~max ~4000 ohms
23 C2 0.47 microfarads
24 R6 13.3 kohms.
26 The thermlstors 82 and 83 in this LBO 40 were GB43Vl devices, manufactured
27 by Penwal Electronics, Farmingham, Mass. An l.BO for operating with 24 and
28 26-gauge ~wisted-pair telephone cable was similar, except that element valuss
29 were changed ~o ~ailor impcdance characteristics o the C~N's to those of
31
- 14 _
,
~ 3~; L-468
¦ the l:ine. The CRN's for the LB0 28 were also similar to the above, except
2 ¦ that element values were changed for operating over a different frequency
3 ¦ band.
4 ¦ The LB0 40 in the abova example was designed to operate at
5 ¦ nominal half-span spacing. If the subscriber ~erminal 12 including LB0 40
¦ is located at exactly half-span, the loss characteristic of line 11
¦ corresponds to curve 14 in FIG. 2. ~le DC error voltage eS4 on line 54 in
¦ ~his instance is 0 volts, or example, and ~he ~hermis~ors 82 and 83 provide
resistances that are equal to Re such that the impedance characteristic of
101 the LB0 is flat as is ~he net loss characteristic of ~he line.
If the length of cable pair 11 is greater than half-span, the loss
I characteristic thereof may c~rrespond to that of curve 16. This means that
131 the error voltage on line 54 decreases or is negative and causes the
14¦ collector currents iC2 and ic3 to decrease ~nd increase, for causing the
151 terminating resistances R82 and R83 of thermistors 82 and 83 to increase
16¦ and deerease, respectively. The impedance ~harac~eris~ics of networks 71
171 and 72 are thereore generally similar to cu~ves 67 and 65, respectively,
18 ¦ such that LB0 40 af0ctively adds positive gain to the line loss to make
19 the net loss oharacteris~ic 1at. Conversely, if the len~th of line 11 is
less than hal-span, corresponding to a loss characteristic such as curve
21 15, a positive error voltage on line 54 causes the collector current iC2
2~ to increa~e so as to decrease the assoc.iated resis~ance o thermistor 82.
The di~erential opera~ion of amplifiar 80 then causes the resistance of
2~ th~rmistor 83 to increase accordin~ly. In this instance~ the impedance
characteristlcs of the networks 71 and 72 are generally similar to ~he
26 curves 65 and G7s respectively, such that the network 40 in this instance
27 adds positive attenuation or additional loss to the signal on line 39 in
28 order ts make the net loss characteristic of the system flat.
29
32 - 15 -
,. .
~ 1 ~ 6 ~ S a ~ L-46~ ¦
1 Although this invQntion is disclosed in relation to a preferred
embodiment thereof, variations and modifications will be apparent to those
3 skilled in the art, without departing from the spirit o~ this invention.
4 For exa~ple, the CRN's may be more complex devices than are illustrated
in FIGS. ~ and 7. Also, the CRN's may comprise lattice structures instead
6 of bridged-T type devices. Furthermore, the inverse networks may comprise
7 groups o~ elements other than and/or more complex than ~hose men~ioned above.
Additionally, the amplifier Ql may be a bootstrap or Darlington compound
and the CRN's may be in other than the collector or emitter circuits of a
transistor. An alternate structure in FIG. 8 includes a pair of CRN's 87
11 and 88 associated with separate operational ampliier circuits 89 ~nd 90.
12 The C~N 87 is in the forward gain loop of ampliieT 89, whereas the other
13 C~N 88 is in ~he feedback loop of amplifier 90. Both of these C2N's 87 and
14 88 s~ill require ~omplementary impedance characteristics. In this
arrangemen~, the CRN's are again terminated by ~ariable resistors having
16 resistances varying inversely. Additionally, although this invention is
17 described in relation to a system including pre~mphasis, post-emphasis
18 could also be employed. Further, the net voltaee gain o amplifier 70 may
19 be made to more nearly approxima~e ~he reciprocal o ~he line loss a~
~20 high ~requencies by adding a small resistance in series with the capacitor
Zl Cl. To keep the integrity of the constant resistance network design,
22 it then becomes necessary to add a large resistance in parallel with ~he
23 inductor Ll. The product o~ these addi~ional resistances is also
24 approxlmately equal to Ro2. In the above examyle, the small series
26 resistance and large shunt resistance were 121 and 6800 ohms, respectively.
The scope of this invention is therefore to be determined rom the att~ched
27 claims rather 1:han from the above detailed descriptions of preferred
28 embodimen~s thereof.
2~
:
31 - 1$
.
